Abstract
One of the central problems in nuclear physics is the description of nuclei as systems of nucleons interacting via realistic potentials. There are two main aspects of this problem: 1) specification of the Hamiltonian, and 2) calculation of the ground (or excited) states of nuclei with the given interaction. Realistic interactions must contain botn two- and three-nucleon potentials and these potentials have a complicated non-central operator structure consisting, for example, of spin, isospin and tensor dependences. This structure results in formidable many-body problems in the computation of the ground states of nuclei.
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